2022ApJ...927...84Z


Query : 2022ApJ...927...84Z

2022ApJ...927...84Z - Astrophys. J., 927, 84-84 (2022/March-1)

Diagnosing the Circumburst Environment with Multiband Gamma-Ray Burst Radio Afterglows.

ZHANG B., LIU L.-D., SUN T.-R., LYU F. and WU X.-F.

Abstract (from CDS):

It has been widely recognized that gamma-ray burst (GRB) afterglows arise from interactions between the GRB outflow and circumburst medium, while their evolution follows the behaviors of relativistic shock waves. Assuming the distribution of circumburst medium follows a general power-law form, that is, n = A * R –k , where R denotes the distance from the burst, it is obvious that the value of the density-distribution index k can affect the behaviors of the afterglow. In this paper, we analyze the temporal and spectral behaviors of GRB radio afterglows with arbitrary k values. In the radio band, a standard GRB afterglow produced by a forward shock exhibits a late-time flux peak, and the relative peak fluxes, as well as peak times at different frequencies, show dependencies on k. Thus, with multiband radio-peak observations, one can determine the density profile of the circumburst medium by comparing the relations between peak flux/time and frequency at each observing band. Also, the effects of transrelativistic shock waves, as well as jets in afterglows, are discussed. By analyzing 31 long and 1 short GRB with multiband data of radio afterglows, we find that nearly half of them can be explained with a uniform interstellar medium (k = 0), ∼1/5 can be constrained to exhibiting a stellar-wind environment (k = 2), while less than ∼1/3 of the samples show 0 < k < 2.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Burst astrophysics

Simbad objects: 34

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Number of rows : 34
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
3 Fermi bn140304557 gB 02 02 33.90 +33 28 27.9           ~ 106 0
4 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
5 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
6 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
7 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
8 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
9 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
10 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
11 GRB 141121A gB 08 10 40.68 +22 13 02.7           ~ 108 0
12 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
13 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
14 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
15 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
16 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
17 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
18 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
19 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
20 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
21 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
22 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
23 GRB 970828 gB 18 08 31.6 +59 18 51           ~ 353 1
24 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
25 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
26 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
27 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
28 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
29 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 248 1
30 GRB 010921 gB 22 55 59.90 +40 55 52.9           ~ 173 1
31 GRB 111215A gB 23 18 13.33 +32 29 38.5           ~ 68 0
32 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0
33 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1
34 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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